| (84) |
Designated Contracting States: |
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AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL
NO PL PT RO RS SE SI SK SM TR |
| (43) |
Date of publication of application: |
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30.10.2013 Bulletin 2013/44 |
| (73) |
Proprietor: Xieon Networks S.à.r.l. |
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1748 Luxemburg (LU) |
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| (72) |
Inventors: |
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- GOTTWALD, Erich
83607 Holzkirchen (DE)
- ROHDE, Harald
81673 München (DE)
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| (74) |
Representative: Liesegang, Eva |
|
Boehmert & Boehmert
Anwaltspartnerschaft mbB
Patentanwälte Rechtsanwälte
Pettenkoferstrasse 20-22 80336 München 80336 München (DE) |
| (56) |
References cited: :
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- HUAN JIANG ET AL: "All-Optical NRZ-OOK to BPSK Format Conversion in an SOA-Based Nonlinear
Polarization Switch", IEEE PHOTONICS TECHNOLOGY LETTERS, IEEE SERVICE CENTER, PISCATAWAY,
NJ, US, vol. 19, no. 24, 15 December 2007 (2007-12-15), pages 1985-1987, XP011197967,
ISSN: 1041-1135, DOI: 10.1109/LPT.2007.909687
- PLEUMEEKERS U ET AL: "All-optical wavelength conversion and broadcasting to eight
separate channels by a single semiconductor optical amplifier delay interferomet",
OPTICAL FIBER COMMUNICATIONS CONFERENCE. (OFC). POSTCONFERENCE TECHNICAL DIGEST. POSTDEADLINE
PAPERS (IEEE CAT. NO.02CH37339) OPT SOC. AMERICA WASHINGTON, DC, USA; [TRENDS IN OPTICS
AND PHOTONICS SERIES. (TOPS)],, vol. TOPS. VOL. 70, 17 March 2002 (2002-03-17), pages
596-597, XP010618002, DOI: 10.1109/OFC.2002.1036585 ISBN: 978-1-55752-701-1
- THEVENAZ L ET AL: "Wideband delays generated in an all-optical tunable delay line,
preserving signal wavelength and bandwidth", COMPTES RENDUS - PHYSIQUE, ELSEVIER,
PARIS, FR, vol. 10, no. 10, 1 December 2009 (2009-12-01), pages 1008-1013, XP026862233,
ISSN: 1631-0705 [retrieved on 2009-12-31]
- NIZAM M H M ET AL: "WASPNET-a wavelength switched photonic network for telecommunication
transport", 19980617, 17 June 1998 (1998-06-17), pages 3/1-3/6, XP006504154,
- JAAFAR M H ELMIRGHANI ET AL: "All-Optical Wavelength Conversion: Technologies and
Applications in DWDM Networks", IEEE COMMUNICATIONS MAGAZINE, IEEE SERVICE CENTER,
PISCATAWAY, US, vol. 38, no. 3, 1 March 2000 (2000-03-01), pages 86-92, XP011091248,
ISSN: 0163-6804
- ASTAR W ET AL: "10 Gbit/s RZ-OOK to BPSK format conversion by cross-phase modulation
in single semiconductor optical amplifier", ELECTRONICS LETTERS, IEE STEVENAGE, GB,
vol. 42, no. 25, 7 December 2006 (2006-12-07), pages 1472-1474, XP006027794, ISSN:
0013-5194, DOI: 10.1049/EL:20062615
- TERJI DURHUUS ET AL: "All-Optical Wavelength Conversion by Semiconductor Optical Amplifiers",
JOURNAL OF LIGHTWAVE TECHNOLOGY, IEEE SERVICE CENTER, NEW YORK, NY, US, vol. 14, no.
6, 1 June 1996 (1996-06-01), XP011028535, ISSN: 0733-8724
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[0001] The invention relates to an optical network component and to a method for processing
data in an optical network. Also, a transmitter comprising at least one such optical
network component is suggested.
[0002] Optical transmitters, in particular coherent data optical transmitters, with phase
modulation are known.
[0004] In other words, the SOA does a conversion from an amplitude modulated signal into
a phase modulated signal.
[0005] Hence, at least one (e.g., tunable) single mode laser can feed a light beam to an
amplitude modulator, e.g., an electro absorption modulator (EAM), and the amplitude
modulated output is further conveyed to an SOA which serves as an amplitude to phase
modulation converter.
[0006] However this scenario bears the disadvantage that the phase modulated signal provided
by the SOA still contains a residual amplitude modulation portion.
[0011] The use of semiconductor optical amplifiers in wavelength converters is also described
in
J.M.H. Elmirghani, "All-Optical Wavelength Conversion: Technologies and Applications
in DWDM Networks", IEEE Communications Magazine, Vol. 38, March 2000, pages 86 to
92;
W. Astar and G. M. Carter, "10 Gbit/s RZ-OOK to BPSK Format Conversion by Cross-Phase
Modulation in Single Semiconductor Optical Amplifier", Electronic Letters Vol. 42,
No. 25, December 2006, pages 1472 to 1474; and
T. Durhuus et al, "All-Optical Wavelength Conversion by Semiconductor Optical Amplifiers",
Journal of Lightwave Technology Vol. 14, No. 6, June 1996, page 942 to 954.
[0012] The problem to be solved is to overcome this disadvantage and to provide a solution
to generate an amplified phase modulated signal in particular utilizing low-cost components.
[0013] This problem is solved according to the features of the independent claims. Further
embodiments result from the depending claims.
[0014] In order to overcome this problem, an optical network component is provided according
to independent claims 1 and 3..
[0015] It is noted that the amplitude modulated and the semiconductor optical amplifier
can be supplied by the same light source. It is also noted that the output of the
amplitude modulator can convey a light beam in opposite direction to the output of
the semiconductor optical amplifier (i.e. the light beam to the semiconductor optical
amplifier is conveyed from the light source to its input).
[0016] It is in particular an embodiment that an input of the amplitude modulator is connected
to the light source.
[0017] This solution allows for an efficient conversion of an amplitude modulated signal
into a phase modulated signal and suppresses the amplitude modulated portion in this
phase modulated signal. This concept does not require a chirp-free modulator and may
be utilized with commonly available and non expensive parts. Also, only a single light
source suffices and the semiconductor optical amplifier provides two functionalities,
i.e. an amplification of the optical signal as well as a conversion from the amplitude
into the phase modulated signal.
[0018] In another embodiment, the light source comprises a laser, in particular at least
one laser diode.
[0019] In a further embodiment, the light source comprises an isolator.
[0020] Instead of the isolator, a combination of a quarter wave plate and a polarizer can
be used.
[0021] It is also an embodiment that the amplitude modulator is an electro absorption modulator
(EAM), in particular a reflective electro absorption modulator (REAM).
[0022] The semiconductor optical amplifier may convey the phase modulated signal with the
suppressed amplitude modulated portion via the circulator to the optical fiber, in
particular to a receiver.
[0023] In an alternative scenario, the semiconductor optical amplifier may convey the phase
modulated signal with the suppressed amplitude modulated portion via the splitter
to the optical fiber, in particular to a receiver, which is connected to the optical
fiber.
[0024] According to another embodiment, the output of the semiconductor optical amplifier
is connected via said splitter and via an attenuator, in particular a variable attenuator,
to the optical fiber.
[0025] In yet another embodiment, the semiconductor optical amplifier is at least temporarily
operated in a saturation mode.
[0026] The semiconductor optical amplifier can be operated in its saturation mode in order
to obtain an efficient phase modulated signal based on the amplitude modulated signal
fed to this semiconductor optical amplifier.
[0027] The problem is also solved by a transmitter comprising at least one optical network
component as described herein.
[0028] The problem mentioned above is further solved by a method for processing data in
an optical network according to independent claims 9 and 10.
[0029] It is noted that the input and the output of the semiconductor optical amplifier
can also be regarded as a first port and a second port.
[0030] According to claim 9, the amplitude modulated signal is conveyed via a circulator
to the semiconductor optical amplifier.
[0031] Pursuant to an alternative embodiment according to claim 10, the amplitude modulated
signal is conveyed via a splitter to the semiconductor optical amplifier.
[0032] It is also an embodiment that the semiconductor optical amplifier is operated in
a saturation mode.
[0033] In the saturation mode, the semiconductor optical amplifier operates at its maximum
level of amplification.
[0034] Furthermore, the problem stated above is solved by a communication system comprising
at least one device as described herein.
[0035] Embodiments of the invention are shown and illustrated in the following figures:
- Fig.1
- shows a schematic diagram of an optical transmitter with a semiconductor optical amplifier
converting an amplitude modulated signal into a phase modulated signal and providing
a reduced level of the amplitude modulated signal at its output;
- Fig.2
- shows an alternative embodiment of the transmitter according to Fig.1.
[0036] The solution provided in particular suggests two arrangements with (at least) one
laser source avoiding residual amplitude modulation. Also, the approach does not require
a chirp-free modulator.
[0037] Fig.1 shows a schematic diagram of an optical transmitter. A laser (preferably with an
isolator) 101 conveys a light beam via a power splitter 102 to an electro absorption
modulator EAM 103 and to a semiconductor optical amplifier SOA 104. The EAM 103 modulates
the light beam with an electrical signal (amplitude modulation) and conveys the modulated
signal to a circulator 105. The circulator 105 conveys this amplitude modulated signal
to the SOA 104. As the light beam is also conveyed from the power splitter 102 to
the SOA 104, both light signals arriving at the SOA 104 result in a phase modulated
signal, wherein the amplitude modulated signal is suppressed based on the SOA's self
phase modulation (SPM). It is noted that the SOA 104 preferably operates in a saturation
mode. The phase modulated signal without a (significant) amplitude modulated portion
is conveyed from the SOA 104 to the circulator 105 and from there across an optical
fiber (indicated by an arrow 106) to a receiver (not shown in Fig.1).
[0038] The amplitude modulated signal is suppressed by a "counter propagating wave" Kerr
effect, wherein the AM modulated light beam originates at the same laser source 101
as does the phase modulated output signal.
[0039] This solution has the advantage of a cost efficient setup that may utilize commonly
available components (no expensive special equipment is required). A chirp of the
modulator (EAM 103) is negligible. The phase modulated output signal provided by such
transmitter has no or only a minimum residual amplitude modulated portion. It is also
an advantage that compared to cross phase modulation (XPM) solutions, only a single
light source (instead of two light sources) is required. The SOA 104 provides two
different functionalities, i.e. an optical amplification and the conversion from amplitude
to phase modulation.
[0040] Fig.2 shows an alternative embodiment with a light source (laser 201) conveying a light
beam to a SOA 202 which further is connected to a 2x2 power splitter 203. The splitter
203 is further connected to a reflective electro absorption modulator REAM 204 and
to a variable attenuator 205.
[0041] The SOA 202 conveys the phase modulated signal via the splitter 203 to the REAM 204
where it is amplitude modulated with an electrical signal. The amplitude (and phase)
modulated signal is then fed back to the splitter 203 and to the SOA 202. This amplitude
and phase modulated signal can also be monitored at the other port of the splitter
203, indicated by an arrow 206. The SOA 202 obtaining the signal from the splitter
203 converts the amplitude modulation to a phase modulation and suppresses (or at
least reduces) the amplitude modulation portion. The resulting (mainly) phase modulated
signal is then fed via the splitter 203 to the variable attenuator 205 (optional)
and conveyed (indicated by an arrow 207) via an optical fiber to a receiver (not shown
in Fig.2).
[0042] In addition to the advantages stated above with regard to Fig.1, this solution shown
in Fig.2 is very cost-efficient, because no circulator is required and of the efficient
implementation of the REAM 204. In addition, the SOA 202 can be used as an amplifier
for the amplitude modulated signal, which reduces the laser power requirement and/or
the modulation index of the REAM 204.
[0043] In the embodiments of Fig.1 and Fig2, a fraction of the emitted light is reflected
backwards to the light source (laser, e.g., laser diode). In order to avoid disturbance
of the light source by back-scattering especially in terms of spectral properties,
the light source may contain an optical isolator. Instead of an optical isolator a
combination of polarizer and a quarter wave plate can be used as described, e.g.,
in
US 2002/0118904 A1.
List of Abbreviations:
[0044]
- AM
- amplitude modulation
- EAM
- electro absorption modulator
- PM
- phase modulation
- REAM
- reflective electro absorption modulator
- SOA
- semiconductor optical amplifier
- XPM
- cross phase modulation
- SPM
- self phase modulation
List of references:
[0045]
- 101
- laser (with an optional isolator); also: light source
- 102
- splitter, in particular power splitter
- 103
- EAM
- 104
- SOA
- 105
- circulator
- 106
- output signal (to be conveyed via optical fiber)
- 201
- laser (with an optional isolator); also: light source
- 202
- SOA
- 203
- splitter
- 204
- REAM
- 205
- variable attenuator (optional)
- 206
- monitoring signal (comprising AM and PM portions)
- 207
- output signal (to be conveyed via optical fiber)
1. An optical network component
- comprising a light source (101), an amplitude modulator (103), and a semiconductor
optical amplifier (104) with an input and an output,
- wherein the input is connected to the light source (101); and
- wherein the output is connected via a circulator (105) to an output of the amplitude
modulator (103),
- wherein the semiconductor optical amplifier (104) converts an amplitude modulated
signal from the amplitude modulator (103) to a phase modulated signal and provides
the phase modulated signal at its output; and
- wherein the output of the semiconductor optical amplifier (104) is connected to
an optical fiber (106) via said circulator (105);
characterized in that:
the light source (101) is connected via a splitter (102) to the input of the semiconductor
optical amplifier (104) and to the amplitude modulator (103).
2. The optical network component according to claim 1, wherein the amplitude modulator
is an electro absorption modulator (103).
3. An optical network component
- comprising a light source (201), an amplitude modulator (204), and a semiconductor
optical amplifier (202) with an input and an output,
- wherein the input is connected to the light source (201); and
- wherein the output is connected to the amplitude modulator (204),
- wherein the semiconductor optical amplifier (202) converts an amplitude modulated
signal from the amplitude modulator (204) to a phase modulated signal and provides
the phase modulated signal at its output; and
characterized in that:
- the output of the semiconductor optical amplifier (202) is connected via a splitter
(203) to the amplitude modulator (204), wherein the amplitude modulator is a reflective
electro absorption modulator (204); and
- the output of the semiconductor optical amplifier (202) is connected via said splitter
(203) to an optical fiber (207).
4. The optical network component according to claim 3, wherein the output of the semiconductor
optical amplifier (202) is connected via said splitter (203) and via an attenuator,
in particular a variable attenuator (205), to the optical fiber (207).
5. The optical network component according to any of the preceding claims, wherein the
light source comprises a laser (101, 201), in particular at least one laser diode.
6. The optical network component according to claim 5, wherein the light source (101;
201) comprises an isolator.
7. The optical network component according to any of the preceding claims, wherein the
semiconductor optical amplifier (104; 202) is adapted to at least temporarily operate
in a saturation mode.
8. A transmitter comprising at least one optical network component according to any of
the preceding claims.
9. A method for processing data in an optical network,
- wherein an amplitude modulated signal is conveyed via a circulator (105) to an output
of a semiconductor optical amplifier (104);
- wherein a light beam is conveyed to an input of the semiconductor optical amplifier
(104);
- wherein the semiconductor optical amplifier (104) converts the amplitude modulated
signal to a phase modulated signal and provides the phase modulated signal at its
output, said output being connected to an optical fiber (106) via said circulator
(105);
characterized by a step of conveying said light beam via a splitter (102) to the input of the semiconductor
optical amplifier (104) and to the amplitude modulator (103).
10. A method for processing data in an optical network,
- wherein an amplitude modulated signal is conveyed to an output of a semiconductor
optical amplifier (202);
- wherein a light beam is conveyed to an input of the semiconductor optical amplifier
(202),
- wherein the semiconductor optical amplifier (202) converts the amplitude modulated
signal to a phase modulated signal and provides the phase modulated signal at its
output; characterized in that:
- the phase modulated signal is amplitude modulated with an electrical signal;
- the amplitude modulated signal is fed back to the semiconductor optical amplifier
(204) via a splitter (203); and
- the phase modulated signal is provided to an optical fiber (207) via said splitter
(203).
11. The method according to claim 10, wherein the semiconductor optical amplifier (104;
202) is operated in a saturation mode.
1. Optische Netzwerkkomponente
- mit einer Lichtquelle (101), einem Amplitudenmodulator (103) und einem optischen
Halbleiterverstärker (104), der einen Eingang und einen Ausgang aufweist,
- wobei der Eingang mit der Lichtquelle (101) verbunden ist, und
- der Ausgang über einen Zirkulator (105) mit einem Ausgang des Amplitudenmodulators
(103) verbunden ist,
- wobei der optische Halbleiterverstärker (104) ein amplitudenmoduliertes Signal von
dem Amplitudenmodulator (103) in ein phasenmoduliertes Signal umwandelt und das phasenmodulierte
Signal an seinem Ausgang bereitstellt, und
- wobei der Ausgang des optischen Halbleiterverstärkers (104) über den Zirkulator
(105) mit einer optischen Faser (106) verbunden ist,
dadurch gekennzeichnet, dass
- die Lichtquelle (101) über einen Splitter (102) mit dem Eingang des optischen Halbleiterverstärkers
(104) und dem Amplitudenmodulator (103) verbunden ist.
2. Optische Netzwerkkomponente nach Anspruch 1, wobei der Amplitudenmodulator ein Elektro-Absorptions-Modulator
(103) ist.
3. Optische Netzwerkkomponente
- mit einer Lichtquelle (201), einem Amplitudenmodulator (204) und einem optischen
Halbleiterverstärker (202), der einen Eingang und einen Ausgang aufweist,
- wobei der Eingang mit der Lichtquelle (201) verbunden ist, und
- wobei der Ausgang mit dem Amplitudenmodulator (204) verbunden ist,
- wobei der optische Halbleiterverstärker (202) ein amplitudenmoduliertes Signal von
dem Amplitudenmodulator (204) in ein phasenmoduliertes Signal umwandelt und das phasenmodulierte
Signal an seinem Ausgang bereitstellt,
dadurch gekennzeichnet, dass
- der Ausgang des optischen Halbleiterverstärkers (202) über einen Splitter (203)
mit dem Amplitudenmodulator (204) verbunden ist, wobei der Amplitudenmodulator ein
reflektiver Elektro-Absorptions-Modulator (204) ist, und
- der Ausgang des optischen Halbleiterverstärkers (202) über den Splitter (203) mit
einer optischen Faser (207) verbunden ist.
4. Optische Netzwerkkomponente nach Anspruch 3, wobei der Ausgang des optischen Halbleiterverstärkers
(202) über den Splitter (203) und über ein Dämpfungsglied, insbesondere ein variables
Dämpfungsglied (205), mit der optischen Faser (207) verbunden ist.
5. Optische Netzwerkkomponente nach einem der vorangehenden Ansprüche, wobei die Lichtquelle
einen Laser (101; 201) umfasst, insbesondere wenigstens eine Laserdiode.
6. Optische Netzwerkkomponente nach Anspruch 5, wobei die Lichtquelle (101; 201) einen
Isolator umfasst.
7. Optische Netzwerkkomponente nach einem der vorangehenden Ansprüche, wobei der optische
Halbleiterverstärker (104; 202) dazu eingerichtet ist, wenigstens vorübergehend in
einem Sättigungsmodus zu arbeiten.
8. Sendeeinrichtung mit wenigstens einer optischen Netzwerkkomponente nach einem der
vorangehenden Ansprüche.
9. Verfahren zum Verarbeiten von Daten in einem optischen Netzwerk,
- wobei ein amplitudenmoduliertes Signal über einen Zirkulator (105) zu einem Ausgang
eines optischen Halbleiterverstärkers (104) übertragen wird;
- wobei ein Lichtstrahl zu einem Eingang des optischen Halbleiterverstärkers (104)
übertragen wird;
- wobei der optische Halbleiterverstärker (104) das amplitudenmodulierte Signal in
ein phasenmoduliertes Signal umwandelt und das phasenmodulierte Signal an seinem Ausgang
bereitstellt, wobei der Ausgang mit einer optischen Faser (106) über den Zirkulator
(105) verbunden wird;
gekennzeichnet durch den Schritt des Übertragens des Lichtstrahls über einen Splitter (102) zu dem Eingang
des optischen Halbleiterverstärkers (104) und zu dem Amplitudenmodulator (103).
10. Verfahren zum Verarbeiten von Daten in einem optischen Netzwerk,
- wobei ein amplitudenmoduliertes Signal zu einem Ausgang eines optischen Halbleiterverstärkers
(202) übertragen wird;
- wobei ein Lichtstrahl zu einem Eingang des optischen Halbleiterverstärkers (202)
übertragen wird,
- wobei der optischen Halbleiterverstärker (202) das amplitudenmodulierte Signal in
ein phasenmoduliertes Signal umwandelt und das phasenmodulierte Signal an seinem Ausgang
bereitstellt;
dadurch gekennzeichnet, dass
- das phasenmodulierte Signal eine mit einem elektrischen Signal modulierte Amplitude
ist;
- das amplitudenmodulierte Signal über einen Splitter (203) zu dem optischen Halbleiterverstärker
(204) zurückgespeist wird; und
- das phasenmodulierte Signal über den Splitter (203) einer optischen Faser (207)
zugeführt wird.
11. Verfahren nach Anspruch 10, wobei der optische Halbleiterverstärker (104; 202) in
einem Sättigungsmodus betrieben wird.
1. Composant de réseau optique
comprenant une source de lumière (101), un modulateur d'amplitude (103), et un amplificateur
optique à semi-conducteur (104) ayant une entrée et une sortie,
où l'entrée est connectée à la source de lumière (101) ; et
où la sortie est connectée via un circulateur (105) à une sortie du modulateur d'amplitude
(103),
où l'amplificateur optique à semi-conducteur (104) convertit un signal modulé en amplitude
depuis le modulateur d'amplitude (103) en un signal modulé en phase et délivre le
signal modulé en phase à sa sortie ; et
où la sortie de l'amplificateur optique à semi-conducteur (104) est connectée à une
fibre optique (106) via ledit circulateur (105) ;
caractérisé en ce que :
la source de lumière (101) est connectée via un séparateur (102) à l'entrée de l'amplificateur
optique à semi-conducteur (104) et au modulateur d'amplitude (103).
2. Composant de réseau optique selon la revendication 1, dans lequel le modulateur d'amplitude
est un modulateur d'électro-absorption (103).
3. Composant de réseau optique
comprenant une source de lumière (201), un modulateur d'amplitude (204), et un amplificateur
optique à semi-conducteur (202) ayant une entrée et une sortie,
où l'entrée est connectée à la source de lumière (201) ; et
où la sortie est connectée au modulateur d'amplitude (204),
où l'amplificateur optique à semi-conducteur (202) convertit un signal modulé en amplitude
depuis un modulateur d'amplitude (204) en un signal modulé en phase et délivre le
signal modulé en phase à sa sortie ; et
caractérisé en ce que :
la sortie de l'amplificateur optique à semi-conducteur (202) est connectée, via un
séparateur (203), au modulateur d'amplitude (204), où le modulateur d'amplitude est
un modulateur d'électro-absorption réflectif (204) ; et
la sortie de l'amplificateur optique à semi-conducteur (202) est connectée via ledit
séparateur (203) à une fibre optique (207).
4. Composant de réseau optique selon la revendication 3, dans lequel la sortie de l'amplificateur
optique à semi-conducteur (202) est connectée via ledit séparateur (203) et via un
atténuateur, en particulier un atténuateur variable (205), à la fibre optique (207).
5. Composant de réseau optique selon l'une quelconque des revendications précédentes,
dans lequel la source de lumière comprend un laser (101, 201), en particulier au moins
une diode laser.
6. Composant de réseau optique selon la revendication 5, dans lequel la source de lumière
(101 ; 201) comprend un isolateur.
7. Composant de réseau optique selon l'une quelconque des revendications précédentes,
dans lequel l'amplificateur optique à semi-conducteur (104 ; 202) est conçu pour fonctionner,
au moins temporairement, dans un mode de saturation.
8. Émetteur comprenant au moins un composant de réseau optique selon l'une quelconque
des revendications précédentes.
9. Procédé pour traiter des données dans un réseau optique,
où un signal modulé en amplitude est acheminé via un circulateur (105) vers une sortie
d'un amplificateur optique à semi-conducteur (104) ;
où un faisceau lumineux est acheminé vers une entrée d'un amplificateur optique à
semi-conducteur (104) ;
où l'amplificateur optique à semi-conducteur (104) convertit le signal modulé en amplitude
en un signal modulé en phase et délivre le signal modulé en phase à sa sortie, ladite
sortie étant connectée à une fibre optique (106) via ledit circulateur (105) ;
caractérisé par une étape consistant à acheminer ledit faisceau lumineux via un séparateur (102)
vers l'entrée de l'amplificateur optique à semi-conducteur (104) et vers le modulateur
d'amplitude (103).
10. Procédé pour traiter des données dans un réseau optique,
où un signal modulé en amplitude est acheminé vers une sortie d'un amplificateur optique
à semi-conducteur (202) ;
où un faisceau lumineux est acheminé vers une entrée de l'amplificateur optique à
semi-conducteur (202) ;
où l'amplificateur optique à semi-conducteur (202) convertit le signal modulé en amplitude
en un signal modulé en phase et délivre le signal modulé en phase à sa sortie ;
caractérisé en ce que :
le signal modulé en phase est modulé en amplitude avec un signal électrique ;
le signal modulé en amplitude est renvoyé à l'amplificateur optique à semi-conducteur
(204), via un séparateur (203) ; et
le signal modulé en phase est délivré à une fibre optique (207) via ledit séparateur
(203).
11. Procédé selon la revendication 10, dans lequel l'amplificateur optique à semi-conducteur
(104 ; 202) fonctionne dans un mode de saturation.